全文获取类型
收费全文 | 118篇 |
免费 | 1篇 |
专业分类
化学 | 38篇 |
物理学 | 81篇 |
出版年
2023年 | 1篇 |
2022年 | 1篇 |
2020年 | 4篇 |
2019年 | 5篇 |
2015年 | 1篇 |
2014年 | 2篇 |
2013年 | 4篇 |
2012年 | 4篇 |
2011年 | 7篇 |
2010年 | 5篇 |
2009年 | 3篇 |
2008年 | 4篇 |
2007年 | 4篇 |
2006年 | 3篇 |
2005年 | 4篇 |
2004年 | 4篇 |
2003年 | 3篇 |
2002年 | 2篇 |
2001年 | 4篇 |
2000年 | 2篇 |
1999年 | 3篇 |
1998年 | 7篇 |
1997年 | 5篇 |
1996年 | 1篇 |
1995年 | 1篇 |
1994年 | 3篇 |
1993年 | 1篇 |
1992年 | 2篇 |
1991年 | 2篇 |
1989年 | 2篇 |
1987年 | 1篇 |
1986年 | 2篇 |
1984年 | 2篇 |
1983年 | 1篇 |
1982年 | 4篇 |
1981年 | 1篇 |
1980年 | 1篇 |
1979年 | 2篇 |
1978年 | 2篇 |
1977年 | 1篇 |
1976年 | 2篇 |
1973年 | 3篇 |
1971年 | 1篇 |
1970年 | 1篇 |
1968年 | 1篇 |
排序方式: 共有119条查询结果,搜索用时 15 毫秒
1.
The Crystal Structures of the Vanadium Weberites Na2MIIVIIIF7 (MII ? Mn, Ni, Cu) and of NaVF4 At single crystals of the vanadium(III) compounds NaVF4 (a = 790.1, b = 531.7, c = 754.0 pm, β = 101.7°; P21/c, Z = 4), Na2NiVF7 (a = 726.0, b = 1031.9, c = 744.6 pm; Imma, Z = 4) and Na2CuVF7 (a = 717.6, b = 1043.5, c = 754.6 pm; Pmnb, Z = 4) X-ray structure determinations were performed, at Na2MnVF7 (a = 746.7, c = 1821.6 pm; P3221, Z = 6) a new refinement. NaVF4 crystallizes in the layer structure type of NaNbO2F2. The fluorides Na2MIIVF7 represent new orthorhombic (MII ? Ni; Cu) resp. trigonal (MII ? Mn) weberites. The average distances within the [VF6] octahedra of the four compounds are in good agreement with each other and with data of related fluorides (V? F: 193.3 pm). The differences between mean bond lengths of terminal and bridging F ligands are 5% in NaVF4, but less than 1% in the weberites. Details and data for comparison are discussed. 相似文献
2.
3.
4.
Christoph Peschel Stefan van Wickeren Yves Preibisch Verena Naber Denis Werner Lars Frankenstein Dr. Fabian Horsthemke Prof. Dr. Urs Peuker Prof. Dr. Martin Winter Dr. Sascha Nowak 《Chemistry (Weinheim an der Bergstrasse, Germany)》2022,28(22):e202200485
Herein we report on an analytical study of dry-shredded lithium-ion battery (LIB) materials with unknown composition. Samples from an industrial recycling process were analyzed concerning the elemental composition and (organic) compound speciation. Deep understanding of the base material for LIB recycling was obtained by identification and analysis of transition metal stoichiometry, current collector metals, base electrolyte and electrolyte additive residues, aging marker molecules and polymer binder fingerprints. For reversed engineering purposes, the main electrode and electrolyte chemistries were traced back to pristine materials. Furthermore, possible lifetime application and accompanied aging was evaluated based on target analysis on characteristic molecules described in literature. With this, the reported analytics provided precious information for value estimation of the undefined spent batteries and enabled tailored recycling process deliberations. The comprehensive feedstock characterization shown in this work paves the way for targeted process control in LIB recycling processes. 相似文献
5.
We present a formalism for treating the problem of impurities in a lattice of magnetic rare earth ions. Latter are subject to a crystalline field and special attention is paid to non-Kramers ions in a singlet ground state. Our calculations are restricted to the paramagnetic regime. We derive the conditions for magnetic localized modes to occur and discuss the appearance of local magnetic instabilities. It is shown that the impurity effects are especially large if the system is close to a magnetic phase transition. Furthermore we compute the influence of impurities on the magnetic transition temperature. For the case of vacancies or nonmagnetic impurities the dependence of the Curie temperature on impurity concentration is derived. It is demonstrated that small amounts of impurities can often completely suppress magnetic ordering. 相似文献
6.
The interaction of ultrashort laser pulses with opaque droplets in the atmosphere is examined numerically. Intense filaments resulting from the balance between self-focusing and ionization of air molecules are shown to be robust against obscurants sized up to 2/3 of the filament diameter. (3D+1)-dimensional numerical simulations confirm recent experimental data [F. Courvoisier et al., Appl. Phys. Lett. 83, 213 (2003)]. The filament is rapidly rebuilt with minimal loss of energy over a few cm after the interaction region. The replenishment of the pulse mainly proceeds from the nonlinear attractor responsible for the formation of a spatial soliton modeling the filament core. 相似文献
7.
B. Ding M. E. Pemble A. V. Korovin U. Peschel S. G. Romanov 《Applied Physics A: Materials Science & Processing》2011,103(3):889-894
Hybrid metal-dielectric photonic crystals assembled from an opal film coated by a gold film are designed in order to realize
optical spectra that emanate from mixing Bloch modes in the opal and surface plasmon polaritons in corrugated gold films.
The photonic crystal provides a spatial template for the gold film profile and modifies the electromagnetic vacuum in the
vicinity to the gold layer. Reflectance spectroscopy was applied to deconvolute the plasmonic and photonic bandgap components
in the optical response of hybrid crystals as opposite to their mixed appearance in the transmission spectra. 相似文献
8.
9.
We discuss the cross sections for neutron scattering and light scattering from a superionic conductor. The motion of the mobile ions is treated as an independent continuous diffusion process through a periodic potential. While this determines the neutron scattering intensity completely, the light scattering is, in addition, strongly influenced by the spatial variation of the polarizability. This leads to selection rules and to differences between the two kinds of spectra. We present a rather complete study of a one-dimensional model which displays the general features of the problem. The results are based on a numerically accurate solution of the corresponding Fokker-Planck equation. 相似文献
10.
A single atom in free space can have a strong influence on a light beam and a single photon can have a strong effect on a
single atom in free space. Regarding this interaction, two conceptually different questions can be asked: can a single atom
fully absorb a single photon and can a single atom fully reflect a light beam. The conditions for achieving the full effect
in either case are different. Here we discuss related questions in the context of an optical resonator. When shaping a laser
pulse properly it will be fully absorbed by an optical resonator, i.e., no light will be reflected and all the pulse energy
will accumulate inside the resonator before it starts leaking out. We show in detail that in this case the temporal pulse
shape has to match the time-reversed pulse obtained by the cavity’s free decay. On the other hand a resonator, made of highly
reflecting mirrors which normally reflect a large portion of any incident light, may fully transmit the light, as long as
the light is narrow band and resonant with the cavity. The analogy is the single atom—normally letting most of the light pass—which
under special conditions may fully reflect the incident light beam. Using this analogy we are able to study the effects of
practical experimental limitations in the atom-photon coupling, such as finite pulses, bandwidths, and solid angle coverage,
and to use the optical resonator as a test bed for the implementation of the quantum experiment. 相似文献